2016
DOI: 10.1007/s11005-016-0921-z
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Characteristic classes of star products on Marsden–Weinstein reduced symplectic manifolds

Abstract: In this note we consider a quantum reduction scheme in deformation quantization on symplectic manifolds proposed by Bordemann, Herbig and Waldmann based on BRST cohomology. We explicitly construct the induced map on equivalence classes of star products which will turn out to be an analogue to the Kirwan map in the Cartan model of equivariant cohomology. As a byproduct we shall see that every star product on a (suitable) reduced manifold is equivalent to a reduced star product.

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Cited by 9 publications
(12 citation statements)
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“…In the case of a regular G-Hamiltonian system Bordemann-Herbig-Waldmann [16] constructed a star product on the reduced symplectic space via homological perturbation of the classical homological reductioná la Batalin-Fradkin-Vilkoviski; see also [35,20]. In [65], Reichert relates the characteristic classes of the unreduced with the reduced star product and thus shows that, under reasonable assumptions on the initial data of the Hamiltonian system, deformation quantization commutes with homological reduction. The method from [16] was generalized by Herbig [37] and Bordemann-Herbig-Pflaum [13] to the singular case under the condition that the zero level set is a complete intersection and that its vanishing ideal is generated by the components of the moment map.…”
Section: The Methodsmentioning
confidence: 99%
“…In the case of a regular G-Hamiltonian system Bordemann-Herbig-Waldmann [16] constructed a star product on the reduced symplectic space via homological perturbation of the classical homological reductioná la Batalin-Fradkin-Vilkoviski; see also [35,20]. In [65], Reichert relates the characteristic classes of the unreduced with the reduced star product and thus shows that, under reasonable assumptions on the initial data of the Hamiltonian system, deformation quantization commutes with homological reduction. The method from [16] was generalized by Herbig [37] and Bordemann-Herbig-Pflaum [13] to the singular case under the condition that the zero level set is a complete intersection and that its vanishing ideal is generated by the components of the moment map.…”
Section: The Methodsmentioning
confidence: 99%
“…As already mentioned in the former section, the purpose of the kinematic Hilbert space is to implement the adjointness and commutation relations among the operators acting on H kin . The question we want to address is then how to formulate the physical inner product, defined through the group averaging procedure (35) in terms of a phase space integration of an appropriate Wigner distribution as depicted in (17). First, one only needs to consider the phase space function corresponding to the non-diagonal density operatorρ(φ, φ ′ ) for the kinematic quantum states φ, φ ′ ∈ D kin ⊂ H kin , that is, a self-adjoint and positive semi-definite operator written asρ…”
Section: The Physical Wigner Distributionmentioning
confidence: 99%
“…for each of the constraints operatorsĈ I = Φ(C I ) ∈ (Ĉ I ) I∈I , related to the classical constraints C I (p, q) by means of the Weyl quantization map (10). Using the integral property of the Wigner distribution (17), and the cyclic phase space behavior of the star-product (24), the physical inner product obtained in (35) can be expressed as…”
Section: The Physical Wigner Distributionmentioning
confidence: 99%
“…The map J is called quantum momentum map and the pairs (⋆, J ) are called equivariant star products, see also [28][29][30] for a classification in the symplectic setting and [11] for the more general Poisson case.…”
Section: Introductionmentioning
confidence: 99%